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3 - World Journal of Gastroenterology

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Sun Y et al . Terahertz pulsed imaging and spectroscopy<br />

referred to as the “THz gap”. In 1975, David Auston at<br />

AT&T Bell Laboratories developed a photoconductive<br />

emitter gated with an optical pulse that led towards bridging<br />

this gap - the ‘Auston switch’ emitted broadband THz<br />

radiation up to 1 mW. A coherent method to detect THz<br />

pulses in the time domain was also proposed [3] . This became<br />

the foundation <strong>of</strong> THz time-domain spectroscopy<br />

(THz-TDS) [4] , since then many improvements in the generation<br />

and detection <strong>of</strong> coherent THz radiation enabled<br />

THz-TDS and imaging techniques to be pioneered for<br />

applications in various fields such as biomedical engineering,<br />

physics, astronomy, security screening, communications,<br />

genetic engineering, pharmaceutical quality control<br />

and medical imaging [5] . In this paper, THz technology is<br />

introduced and some emerging applications in biology<br />

and medicine including molecular spectroscopy, tissue<br />

characterization and skin imaging are presented.<br />

The aim <strong>of</strong> this article is to review the potential <strong>of</strong><br />

THz pulsed imaging and spectroscopy as a promising<br />

diagnostic method. Several unique features make THz<br />

very suitable for medical applications. (1) THz radiation<br />

has very low photon energy, which is insufficient to cause<br />

chemical damage to molecules, or knock particles out<br />

<strong>of</strong> atoms. Thus, it will not cause harmful ionization in<br />

biological tissues; this makes it very attractive for medical<br />

applications; (2) THz radiation is very sensitive to polar<br />

substances, such as water and hydration state. For this<br />

reason, THz waves can provide a better contrast for s<strong>of</strong>t<br />

tissues than X-rays; (3) THz-TDS techniques use coherent<br />

detection to record the THz wave’s temporal electric<br />

fields, which means both the amplitude and phase <strong>of</strong> the<br />

THz wave can be obtained simultaneously. The temporal<br />

waveforms can be further Fourier transformed to give the<br />

spectra. This allows precise measurements <strong>of</strong> the refractive<br />

index and absorption coefficient <strong>of</strong> samples without<br />

resorting to the Kramers-Kronig relations; and (4) The<br />

energy <strong>of</strong> rotational and vibrational transitions <strong>of</strong> molecules<br />

lies in the THz region and intermolecular vibrations<br />

such as hydrogen bonds exhibit different spectral characteristics<br />

in the THz range. These unique spectral features<br />

can be used to distinguish between different materials or<br />

even isomers.<br />

PRINCIPLES OF THZ PULSED IMAGING<br />

AND SPECTROSCOPY<br />

THz systems<br />

Over the past two decades, technology for generating and<br />

detecting THz radiation has advanced considerably. Several<br />

commercialized systems are now available [6-10] and THz<br />

systems have been set up by many groups all over the<br />

world. According to the laser source used, THz systems<br />

can be divided into two general classes: continuous wave<br />

(CW) and pulsed.<br />

A typical CW system can produce a single fixed frequency<br />

or several discrete frequency outputs. Some <strong>of</strong><br />

them can be tunable. Generation <strong>of</strong> CW THz radiation<br />

can be achieved by approaches such as photomixing [11] ,<br />

WJR|www.wjgnet.com<br />

Laser diode1<br />

Laser diode2<br />

BS<br />

Emitter<br />

cw THz<br />

Sample<br />

Detector<br />

Delay<br />

Figure 1 Schematic illustration <strong>of</strong> a continuous wave THz imaging system<br />

in transmission geometry.<br />

Vitesse<br />

femtosecond<br />

pulsed laser<br />

Delay stage<br />

Probe<br />

beam<br />

Sample<br />

Quartz imaging plate<br />

Photoconductive<br />

emitter<br />

free-electron lasers [12] and quantum cascade lasers [13] .<br />

Figure 1 illustrates a CW THz system which photomixes<br />

two CW lasers in a photoconductor as an example [14] . The<br />

mixing <strong>of</strong> two above-bandgap (visible or near-infrared)<br />

wavelengths produces beating, which can modulate the<br />

conductance <strong>of</strong> a photoconductive switch at the THz<br />

difference frequency. The photomixing device is labeled<br />

“emitter” in Figure 1. Since the source spectrum <strong>of</strong> the<br />

CW system is narrow and sometimes only the intensity<br />

information is <strong>of</strong> interest, the data structures and postprocessing<br />

are relatively simple. It is possible now to<br />

drive a whole CW system by laser diodes and thus it can<br />

be made compact and inexpensive. However, due to the<br />

limited information that CW systems provide, they are<br />

sometimes confined to those applications where only features<br />

at some specific frequencies are <strong>of</strong> interest.<br />

In pulsed systems, broadband emission up to several<br />

THz can be achieved. Currently, there are a number <strong>of</strong><br />

ways to generate and detect pulsed THz radiation, such<br />

as ultrafast switching <strong>of</strong> photoconductive antennas [3] , rectification<br />

<strong>of</strong> optical pulses in crystals [15] , rapid screening<br />

<strong>of</strong> the surface field via photoexcitation <strong>of</strong> dense electron<br />

hole plasma in semiconductors [16] and carrier tunneling in<br />

coupled double quantum well structures [17] . Among them,<br />

the most established approaches based on photoconductive<br />

antennas, where an expensive femtosecond laser is<br />

required and configured as shown in Figure 2. Unlike CW<br />

THz imaging system, coherent detection in pulsed THz<br />

imaging techniques can record THz waves in the time do-<br />

56 March 28, 2011|Volume 3|Issue 3|<br />

30°<br />

Photoconductive<br />

detector<br />

Pump beam<br />

Figure 2 Schematic illustration <strong>of</strong> a pulsed THz imaging system with reflection<br />

geometry.

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